Electronic Devices Ninth Edition Floyd Chapter 15

Basic filter Responses Summary Basic filter Responses A filter is a circuit that passes certain frequencies and rejects all others. The passband is the range of frequencies allowed through the filter. The critical frequency defines the end (or ends) of the passband. Basic filter responses are: Low-pass High-pass Band-pass Band-stop

The Basic Low-Pass Filter Summary The Basic Low-Pass Filter The low-pass filter allows frequencies below the critical frequency to pass and rejects other. The simplest low-pass filter is a passive RC circuit with the output taken across C.

The Basic High-Pass Filter Summary The Basic High-Pass Filter The high-pass filter passes all frequencies above a critical frequency and rejects all others. The simplest high-pass filter is a passive RC circuit with the output taken across R.

Summary The Band-Pass Filter A band-pass filter passes all frequencies between two critical frequencies. The bandwidth is defined as the difference between the two critical frequencies. The simplest band-pass filter is an RLC circuit.

Summary The Band-Stop Filter A band-stop filter rejects frequencies between two critical frequencies; the bandwidth is measured between the critical frequencies. The simplest band-stop filter is an RLC circuit.

Summary Active Filters Active filters include one or more op-amps in the design. These filters can provide much better responses than the passive filters illustrated. Active filter designs optimize various parameters such as amplitude response, roll-off rate, or phase response. Chebyshev: rapid roll-off characteristic Butterworth: flat amplitude response Bessel: linear phase response

Summary The Damping Factor The damping factor primarily determines if the filter will have a Butterworth, Chebyshev, or Bessel response. The term pole has mathematical significance with the higher level math used to develop the DF values. For our purposes, a pole is the number of non-redundant reactive elements in a filter. For example, a one-pole filter has one resistor and one capacitor.

Summary The Damping Factor Parameters for Butterworth filters up to four poles are given in the following table. (See text for larger order filters). Butterworth filter values Order Roll-off dB/decade 1st stage 2nd stage Poles DF R1 /R2 1 -20 Optional 2 -40 1.414 0.586 3 -60 1.00 4 -80 1.848 0.152 0.765 1.235 Notice that the gain is 1 more than this resistor ratio. For example, the gain implied by this ratio is 1.586 (4.0 dB).

Two-pole Low-Pass Butterworth Design Summary Two-pole Low-Pass Butterworth Design As an example, a two-pole VCVS Butterworth filter is designed in this and the next two slides. Assume the fc desired is 1.5 kHz. A basic two-pole low-pass filter is shown. Step 1: Choose R and C for the desired cutoff frequency based on the equation By choosing R = 22 kW, then C = 4.8 nF, which is close to a standard value of 4.7 nF. 4.7 nF 22 kW 22 kW 4.7 nF

Two-pole Low-Pass Butterworth Design Summary Two-pole Low-Pass Butterworth Design Step 2: Using the table for the Butterworth filter, note the resistor ratios required. Butterworth filter values Order Roll-off dB/decade 1st stage 2nd stage Poles DF R1 /R2 1 -20 Optional 2 -40 1.414 0.586 3 -60 1.00 4 -80 1.848 0.152 0.765 1.235 Step 3: Choose resistors that are as close as practical to the desired ratio. Through trial and error, if R1 = 33 kW, then R2 = 56 kW.

Two-pole Low-Pass Butterworth Design Summary Two-pole Low-Pass Butterworth Design The design is complete and the filter can now be tested. 4.7 nF You can check the design using Multisim. The Multisim Bode plotter is shown with the simulated response from Multisim. 22 kW 22 kW 4.7 nF 33 kW 56 kW To read the critical frequency, set the cursor for a gain of 1 dB, which is -3 dB from the midband gain of 4.0 dB. The critical frequency is found by Multisim to be 1.547 kHz.

Four-pole Low-Pass Butterworth Design Summary Four-pole Low-Pass Butterworth Design Question: What changes need to be made to change the two-pole low-pass design to a four-pole design? Answer: Add an identical section except for the gain setting resistors. Choose R1-R4 based on the table for a 4-pole design. 3.3 kW The resistor ratio for the 1st section needs to be 0.152 (gain = 1.152); the 2nd section needs to be 1.235 (gain = 2.235). Use standard values if possible. 15 kW 22 kW 12 kW

High-Pass Active Filter Design Summary High-Pass Active Filter Design The low-pass filter can be changed to a high-pass filter by simply reversing the R’s and C’s in the frequency-selective circuit. For the four-pole design, the gain setting resistors are unchanged. Low-pass High-pass 3.3 kW 15 kW 22 kW 12 kW

Summary Bessel Filter Design Butterworth VCVS filters are the simplest to implement. Chebychev and Bessel filters require an additional correction factor to the frequency to obtain the correct fc. Bessel filter parameters are shown here. The frequency determining R’s are divided by the correction factors shown with the gains set to new values. The following slide illustrates a design. Bessel filters Order Roll-off dB/decade 1st stage 2nd stage Correction DF R1 /R2 2 -40 1.272 1.732 0.268 4 -80 1.432 1.916 0.084 1.606 1.241 0.759

Summary Bessel Filter Design Example: Solution: Modify the 4-pole low-pass design for a Bessel response. Solution: Divide the R’s by the correction factors on the Bessel table and change the gain setting resistors to the ratios on the table. Bessel Low-pass Butterworth Low-pass 22 kW 3.3 kW 12 kW 15 kW

Summary Bessel Filter Design You can test the design with Multisim. Although the roll-off is not as steep as other designs, the Bessel filter is superior for its pulse response. The Bode plotter illustrates the response. Bessel Low-pass

Active Band-Pass Filters Summary Active Band-Pass Filters One implementation of a band-pass filter is to cascade high-pass and low-pass filters with overlapping responses. These filters are simple to design, but are not good for high Q designs.

Active Band-Pass Filters Summary Active Band-Pass Filters The multiple-feedback band-pass filter is also more suited to low-Q designs (<10) because the gain is a function of Q2 and may overload the op-amp if Q is too high. Resistors R1 and R3 form an input attenuator network that affect Q and are an integral part of the design. Key equations are:

Active Band-Pass Filters Summary Active Band-Pass Filters The state-variable filter is suited to high Q band-pass designs. It is normally optimized for band-pass applications but also has low-pass and high-pass outputs available. The next slide shows an example of the Multisim Bode plotter with the circuit file that accompanies the text for Example 15-7. The Bode plotter illustrates the high Q response of this type of filter… The Q is given by

Active Band-Pass Filters Summary Active Band-Pass Filters The cursor is set very close to the lower cutoff frequency.

Active Band-Stop Filters Summary Active Band-Stop Filters A band-stop (notch) filter can be made from a multiple feedback circuit or a state-variable circuit. By summing the LP and HP outputs from a state-variable filter, a band-stop filter is formed. The next slide shows an example of the (corrected) Multisim file that accompanies the text for Example 15-8.

Active Band-Stop Filters Summary Active Band-Stop Filters This circuit is based on text Example 15-8, which notches 60 Hz. The response can be observed with the Bode plotter. The cursor is shown on the center frequency of the response.

Summary Filter Measurements Filter responses can be observed in practical circuits with a swept frequency measurement. The test setup for this measurement is shown here. The sawtooth waveform synchronizes the oscilloscope with the sweep generator.

Selected Key Terms Pole Roll-off Damping factor A circuit containing one resistor and one capacitor that contributes -20 dB/decade to a filter’s roll-off. The rate of decrease in gain below or above the critical frequencies of a filter. A filter characteristic that determines the type of response.